EP3830527A1 - Fluid contaminant detection using noise levels in magnetic flow meter sensor signals - Google Patents
Fluid contaminant detection using noise levels in magnetic flow meter sensor signalsInfo
- Publication number
- EP3830527A1 EP3830527A1 EP19735093.7A EP19735093A EP3830527A1 EP 3830527 A1 EP3830527 A1 EP 3830527A1 EP 19735093 A EP19735093 A EP 19735093A EP 3830527 A1 EP3830527 A1 EP 3830527A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- noise
- sensor signal
- contaminant
- flow meter
- noise level
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 239000000356 contaminant Substances 0.000 title claims abstract description 65
- 239000012530 fluid Substances 0.000 title description 7
- 238000001514 detection method Methods 0.000 title description 2
- 239000007788 liquid Substances 0.000 claims abstract description 62
- 238000000034 method Methods 0.000 claims description 53
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 40
- 239000004576 sand Substances 0.000 claims description 13
- 238000013480 data collection Methods 0.000 claims description 10
- 239000007787 solid Substances 0.000 claims description 4
- 238000001914 filtration Methods 0.000 claims description 2
- 230000000737 periodic effect Effects 0.000 claims 1
- 239000007789 gas Substances 0.000 description 33
- 238000010586 diagram Methods 0.000 description 22
- 239000011800 void material Substances 0.000 description 16
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 12
- 238000005096 rolling process Methods 0.000 description 8
- 239000003345 natural gas Substances 0.000 description 6
- 238000004891 communication Methods 0.000 description 4
- 239000000470 constituent Substances 0.000 description 3
- 239000003995 emulsifying agent Substances 0.000 description 3
- 239000003921 oil Substances 0.000 description 3
- 239000003595 mist Substances 0.000 description 2
- 239000011343 solid material Substances 0.000 description 2
- 238000012935 Averaging Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000002596 correlated effect Effects 0.000 description 1
- 230000000875 corresponding effect Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 239000002803 fossil fuel Substances 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 239000008239 natural water Substances 0.000 description 1
- 239000003129 oil well Substances 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
- G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
- G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
- G01F1/588—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters combined constructions of electrodes, coils or magnetic circuits, accessories therefor
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
- G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
- G01F1/60—Circuits therefor
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/74—Devices for measuring flow of a fluid or flow of a fluent solid material in suspension in another fluid
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M3/00—Investigating fluid-tightness of structures
- G01M3/02—Investigating fluid-tightness of structures by using fluid or vacuum
- G01M3/26—Investigating fluid-tightness of structures by using fluid or vacuum by measuring rate of loss or gain of fluid, e.g. by pressure-responsive devices, by flow detectors
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
- G01N27/72—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables
- G01N27/74—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables of fluids
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
- G01N33/26—Oils; Viscous liquids; Paints; Inks
- G01N33/28—Oils, i.e. hydrocarbon liquids
- G01N33/2835—Specific substances contained in the oils or fuels
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
- G01N33/26—Oils; Viscous liquids; Paints; Inks
- G01N33/28—Oils, i.e. hydrocarbon liquids
- G01N33/2835—Specific substances contained in the oils or fuels
- G01N33/2841—Gas in oils, e.g. hydrogen in insulating oils
Definitions
- Oil wells bring fossil-fuels from underground to the surface.
- the output of the well includes a combination of oil, natural gas, water and solid material, such as sand or silt.
- Separators reside on onshore well pads and offshore platforms and are used to separate the oil and natural gas from each other and from the water and solid debris.
- Separators include an inflow pipe that brings the output of the well into the separator, a natural gas output pipe, an oil output pipe and a water output pipe. If the oil level or water level drops too low, it is possible for natural gas to flow into the oil output pipe or the water output pipe. In addition, it is possible for oil or sand to enter the water output pipe. To prevent this, some separators place valves on the oil output pipe and the water output pipe that are designed to close when the oil level or the water level is too low. These valves, however, are susceptible to sticking due to sand and other debris present in the inflow to the separator. It would be useful to determine if gas, oil or sand is present in the water flow and to determine if gas is present in the oil flow.
- a magnetic flow meter includes electrode sensors generating a sensor signal indicative of flow of a liquid through a conduit.
- a noise identification module identifies a noise level in the sensor signal and a contaminant identification module uses the noise level to determine whether there is a contaminant in the liquid in the conduit.
- a drive signal is applied to generate a magnetic field in a conduit carrying a liquid.
- a sensor signal is received from electrodes positioned along the conduit and a noise level in the sensor signal is determined. The noise level is used to determine if the liquid contains a contaminant.
- a process transmitter includes a magnetic coil and electrode sensors configured to generate a sensor signal.
- a noise identification module is configured to determine a level of noise in the sensor signal and a contaminant identification module is configured to identify that a liquid contains a contaminant based on the determined level of noise.
- FIG. 1 is a sectional view of a separator.
- FIG. 2 is a block diagram of a flow meter in accordance with one embodiment.
- FIG. 3 is a graph of a drive signal for a magnetic flow meter.
- FIG. 4 is a graph of a magnetic flow meter sensor signal in response to the drive signal of FIG. 3 for a liquid that does not contain a contaminant.
- FIG. 5 is a graph of a magnetic flow meter sensor signal in response to the drive signal of FIG. 3 for a liquid containing a contaminant.
- FIG. 6 is a graph of the noise level in the magnetic flow meter sensor signal as a function of the gas void fraction in the liquid.
- FIG. 7 is a flow diagram of a method of collecting data in accordance with one embodiment.
- FIG. 8 is a block diagram of elements used in the method of FIG. 7.
- FIG. 9 is a flow diagram of a method of identifying noise levels in a magnetic flow meter sensor signal in accordance with one embodiment.
- FIG. 10 is a block diagram of elements used in the method of FIG. 9.
- FIG. 11 is a flow diagram of a method of identifying a contaminant using noise levels in accordance with one embodiment.
- FIG. 12 is a block diagram of elements used in the method of FIG. 11.
- FIG. 13 provides graphs of Fast Fourier Transforms of magnetic flow meter sensor signals for different percentages of gas void fraction.
- FIG. 14 is an expanded view of one of the graphs of FIG. 13 showing samples used to determine a noise level in the magnetic flow meter sensor signal.
- FIG. 15 are graphs of noise levels in magnetic flow meter sensor signals determined for different ranges of frequencies during an increase in gas void fractions.
- FIG. 16 are graphs of noise levels in magnetic flow meter sensor signals determined for different ranges of frequencies during an increase in oil percentage in a water line.
- FIG. 17 shows graphs of noise levels in magnetic flow meter sensor signals as a function of gas void fractions for two separate flow rates.
- FIG. 18 shows a graph of noise levels in magnetic flow meter sensor signals as a function of oil levels in a water line.
- FIG. 19 shows a graph of noise levels in magnetic flow meter sensor signals as a function of pounds of sand in a water line.
- FIG. 20 is a flow diagram of a method of collecting noise data in accordance with a further embodiment.
- FIG. 21 is a block diagram of the elements used in the method of FIG. 20.
- FIG. 22 is a flow diagram of a method of identifying noise levels in a magnetic flow meter sensor signal in accordance with a further embodiment.
- FIG. 23 is a block diagram of elements used in the method of FIG. 22.
- Embodiments described below provide process transmitters that detect when a conductive liquid carried by a conduit contains a contaminant such as a gas, another liquid or particulates, such as sand, for example.
- the process transmitters make these determinations by monitoring the noise level in a magnetic flow meter’s sensor signal.
- the present inventors have discovered that as the amount of a contaminant in a liquid increases, the noise level of the magnetic flow meter’s sensor signal increases.
- FIG. 1 provides an example environment 100 in which flow meter 104 of the various embodiments may be utilized.
- Environment 100 includes a separator tank 106 that is able to separate an inflow 108 into various constituents including water 110, oil 112, and gas 114.
- Inflow 108 may be from a well head, in some embodiments.
- Separator tank 106 includes an inlet baffle 116 and a quieting baffle 118 that are used to reduce the velocity of inflow 108 to allow the constituents of inflow 108 to separate from each other to form a gas layer 122, an oil layer 124 and a water layer 126.
- a mist pad 120 collects water and oil droplets present in gas layer 122 and causes the collected oil and water to drop into oil layer 124 and water layer 126.
- Oil layer 124 and water layer 126 flow toward a weir 128 that separates oil layer 124 from water layer 126.
- oil layer 124 flows over the top of weir 128 into an oil chamber 130.
- Water layer 126 flows under oil chamber 130 and into a water chamber 132.
- the level of oil in oil chamber 130 is controlled by a liquid level controller 134 and a valve 136. As liquid level controller 134 drops, valve 136 is closed to prevent fluid from flowing through valve 136.
- liquid level controller 134 include a mechanical controller, a pneumatic controller, and an electronic controller. When operating properly, liquid level controller 134 should completely close valve 136 when the oil level drops below the intake of a downcomer 138 thereby preventing gas 114 from flowing through an output oil conduit 140. Preventing gas from flowing through conduit 140 is important since such gas is valuable and can be dangerous if not handled properly.
- liquid level controller 142 The level of water in water chamber 132 is controlled by liquid level controller 142 and valve 144. As the water level in water chamber 132 drops, liquid level controller 142 closes valve 144 to prevent fluids from flowing through output water conduit 146. Liquid level controller 142 may be a mechanical controller, a pneumatic controller, or an electronic controller. By closing valve 144, liquid level controller 142 prevents gas 114 from flowing through conduit 146 when the water 110 in chamber 132 drops below an intake of a downcomer 148. This prevents gas from entering a water storage tank thereby preventing the loss of valuable gas and preventing explosive gases from developing within the water storage tank.
- flow meter 104 detects when a contaminant such as gas, oil or sand is flowing in water conduit 146. Upon detecting that a contaminant is present in the conduit, flow meter 104 can provide an alert message and/or an indication of the amount of contaminant that is in the conduit.
- FIG. 2 provides a schematic diagram of a process transmitter in the form of a magnetic flow meter 200, which is an example of flow meter 104, in accordance with the various embodiments.
- Magnetic flow meter 200 includes a coil driver 202, which drives electrical current through two coils 204 and 206 positioned on opposite sides of a conduit 208. The current in coils 204 and 206 generates a magnetic field 230 that passes through conduit 208. In accordance with most embodiments, the current in coils 204 and 206 is periodically reversed causing the direction of magnetic field 230 to alternate between extending from coil 204 to coil 206 to extending from coil 206 to coil 204.
- Conduit 208 carries a conductive liquid that moves through conduit 208 in a flow direction 210.
- Polar molecules or charged molecules and atoms within the liquid experience a force that is orthogonal to magnetic field 230 due to their movement through magnetic field 230 in flow direction 210.
- positively charged molecules and atoms move in one direction and negatively charged molecules and atoms in an opposite direction.
- Polar molecules align such that the positive end of the molecules all point in one direction and the negative end of the molecules point in the opposite direction.
- Electrodes 212 and 214 are connected to an analog-to-digital convertor 216 in a housing 228.
- Analog-to-digital convertor 216 samples the analog voltage between electrodes 212 and 214 to produce a series of digital samples for a data collection module 218.
- Data collection module 218 selectively stores some or all of the digital samples for use by a flow calculator 220, which uses the magnitude of the digital samples to estimate a flow rate for the liquid. This flow rate is periodically provided to an input/output circuit 224, which transmits the flow rate to a control room along a communication channel, such as a two- wire process loop 226.
- FIG. 3 provides a graph 300 of a square wave drive signal that is applied to coils 204 and 206 to generate the magnetic field in accordance with one embodiment.
- the magnitude of the current is shown along vertical axis 302 and time is shown along horizontal axis 304.
- the current alternates between a positive and a negative current of the same magnitude.
- the drive signal is a sine wave or a multi-step pulsed DC wave such as a 75 Hz square wave superimposed on a 5Hz square wave, for example.
- FIG. 4 provides a graph 400 of a sensor signal generated between electrodes 212 and 214 when a fluid without a contaminant is flowing through conduit 208 and drive signal 300 is applied to coils 204 and 206.
- the voltage between electrodes 212 and 214 is shown on vertical axis 402 in terms of counts generated by analog-to-digital convertor 216.
- Time is shown along horizontal axis 404.
- the voltage alternates between positive and negative values of similar magnitudes and is relatively stable at each positive and negative value.
- FIG. 5 provides a graph 500 of a sensor signal generated between electrodes 212 and 214 when a contaminant is present in the fluid and drive signal 300 is applied to coils 204 and 206.
- the voltage between electrodes 212 and 214 is shown on vertical axis 502 in terms of counts generated by analog-to-digital convertor 216 and time is shown along horizontal axis 504.
- the contaminant causes variations in the sensed voltage during the steady-state portions of drive signal 300. The present inventors refer to these variations in the voltage as noise in the sensor signal.
- FIG. 6 provides graphs 600 and 602 showing the correlation between gas void fractions in a liquid and noise levels in a sensor signal.
- graph 600 shows a change in the gas void fraction over time during an experiment, with axis 604 showing the gas void fraction as a percentage of a volume in the conduit.
- Graph 602 shows the magnitude of the noise in the sensor signal formed during the change in gas void fraction shown in graph 600, with the magnitude of the noise depicted on vertical axis 606.
- FIG. 6 it can be seen that soon after the gas void fraction begins to increase, the magnitude of the noise in the sensor signal also increases.
- the digital values output by analog-to-digital converter 216 are provided to a data collection module 240, which selectively samples and filters the digital values to produce a set of digital values for a noise identification module 242.
- Noise identification module 242 uses the digital values to identify a sequence of noise values, representing the magnitude of the noise in each of a set of time periods or sections of the sensor signal.
- the sequence of noise values is provided to a contaminant /valve chatter identification module 244, which filters the sequence of noise values to remove spikes in the noise and uses the filtered noise values to determine if the liquid contains a contaminant or if a valve in the process system is experiencing valve chatter.
- contaminant/valve chatter identification module 244 optionally provides an estimate of the amount of contaminant in the liquid.
- contaminant/valve chatter identification module 244 sends an alert through I/O circuit 224 and communication channel 226 indicating the contaminant and optionally the estimated amount of the contaminant.
- FIG. 7 provides a flow diagram of a method implemented by data collection module 240 in accordance with one embodiment.
- FIG. 8 provides a block diagram of elements used in the method of FIG. 7.
- analog-to-digital convertor 216 issues an interrupt signal indicating that analog-to-digital convertor 216 has a new digital sample of the sensor signal.
- the digital sample output by analog-to-digital convertor 216 is stored in a rolling or circular buffer 800 at step 702.
- a cycle monitor 802 determines if an end of a half-cycle of the drive signal has been reached, where the end of a half cycle is the point where the drive signal changes polarity. For example, time points 306 and 308 of FIG.
- cycle monitor 802 determines if the end of a half-cycle has been reached by comparing the polarity of the drive signal to the polarity determined at a previous time point to see if the polarity has changed.
- the end of the half-cycle is determined by comparing the latest output value from analog-to-digital convertor 216 and a previous output of analog-to-digital convertor 216 to an average of the output values from analog-to-digital converter 216.
- line 506 represents the average of the output values from analog-to-digital convertor 216.
- Sample 502 is shown to be at the end of a half-cycle 512 and is greater than average 506 while sample 504, the sample immediately after sample 502, is shown to be at the beginning of a next half-cycle 514 and is less than average 506.
- sample 508 is shown to be at the end of half-cycle 514 and is less than average 506 while sample 510, which is immediately after sample 508, is shown to be at the beginning of the next half-cycle 516 and is greater than average 506.
- a sample selection module 806 is triggered to select a percentage of the samples generated during the last half-cycle at step 706.
- the last twenty percent of the samples in the half-cycle are selected. For example, in FIG. 5 the set of samples 520 at the end of half-cycle 512 are selected during a first pass through step 706 and the set of samples 522 at the end of half-cycle 514 are selected during the next pass through step 706.
- the selection of the samples in step 706 is a selection of a portion of the sensor signal for determining a noise level and separate noise levels are determined for each portion of the sensor signal selected with each execution of step 706.
- a square wave is used as the drive signal.
- samples for the last 20% of each half-cycle of the higher-frequency square wave are selected by sample selection module 806. (for example, the 75 Hz square wave when a 75 Hz square wave is superimposed on a 5 Hz square wave to form the pulsed DC wave).
- the drive signal is a sine wave
- a high pass filter is used to by sample selection module 806 to select a subset of the samples for measuring noise.
- the selected samples are then processed in noise identification module 242 using the method of FIG. 9 and the elements in the block diagram of FIG. 10 to identify the level of noise in the selected samples.
- the samples selected by data collection 240 are ready to be processed.
- the samples are applied to a DC filter 1000, which subtracts a DC value from the samples.
- the DC value is an average of the selected samples.
- the DC filtered samples are applied to a high-pass filter 1002, which removes low frequency signals common to sensor signals generated from pure liquids that do not contain a contaminant.
- the level of noise in the filtered signal can be determined using one or more of a standard deviation calculator 1004 in step 906, a range calculator 1006 in step 908, an average movement per step calculator 1008 in step 910 and/or a maximum movement per step calculator 1010 in step 912.
- Standard deviation calculator 1004 determines the standard deviation of the filtered samples and sets the noise level to the standard deviation.
- Range calculator 1006 determines the difference between the largest filtered sample and the smallest filtered sample in the set of samples selected for the half-cycle and sets the noise level to the difference.
- Average movement per step calculator 1008 determines the average difference between successive filtered samples in the set of samples selected for the half-cycle and sets the noise level to this average difference.
- Max movement per step calculator 1010 determines the largest difference between successive filtered samples in the set of samples selected for the half cycle and sets the noise level to this largest difference. In some embodiments, two or more of these noise levels are combined by, for example, averaging the two or more noise levels together.
- FIG. 11 provides a flow diagram of a method of identifying a contaminant for the noise levels in accordance with one embodiment.
- FIG. 12 provides a block diagram of elements used in the method of FIG. 11.
- the noise levels are applied to a median filter 1200 which forms a window of successive noise levels, such as four successive noise levels, and selects the median of those noise levels as the noise level for the window.
- the noise levels output by median filter 1200 are applied to a low pass filter 1202 to remove high-frequency noise.
- the filtered noise levels are applied to a comparator 1204, which compares the filtered noise levels to a threshold 1206. If the filtered noise level does not exceed the threshold, the process of FIG. 11 ends at step 1112. If the filtered noise levels exceed threshold 1206 at step 1104, an alert is sent by alert generation 1212 to a host system through I/O circuit 224 and communication channel 226 at step 1106.
- the filtered noise levels are applied to a contaminant estimator 1210, which estimates the amount of contaminant in the liquid using a noise-to-contaminant function 1208 at step 1108.
- Noise-to- contaminant function 1208 describes the relationship between the filtered noise levels and the amount of contaminant in the liquid and can be determined from experimental data.
- contaminant estimator 1210 can estimate an amount of gas in a liquid, an amount of oil in a liquid and/or an amount of solid particles in a liquid
- contaminant estimator 248 sends the amount of contaminant in the liquid to alert generation 1212, which forwards the amount of contaminant to the host through I/O circuit 224 and communication channel 226.
- a single alert is sent by alert generation 1212 to convey that the liquid contains a contaminant and the amount of the contaminant in the liquid.
- data collection 240 and noise identification 242 identify a noise level in the sensor signal using a frequency-domain analysis of the sensor signal.
- FIG. 13 shows graphs 1300, 1302, 1304, 1306, and 1308 of a Fast Fourier Transform of sensor signals from a magnetic flow meter generated from a liquid flowing at 3 feet per second and containing respective amounts of gas void fractions of 20%, 10%, 5%, 1% and 0%.
- the magnitude of the signal is shown along vertical axis 1310 and frequency is shown along horizontal axis 1312. As shown in FIG. 13, as the gas void fraction increases, the magnitude of the sensor signal increases across all frequencies.
- FIG. 14 shows an expanded view of graph 1300 with dots positioned at each frequency that is used in the noise determination.
- the drive frequency is 5 Hz and values at even and odd multiples of this frequency are not used to determine the noise level.
- dots are not present on graph 1300.
- the noise is distributed across many frequencies as indicated by the graphs of FIG. 15 where three separate graphs 1500, 1502, and 1504 of noise versus time are shown for an increase in gas void fraction from zero to thirty percent using three respective frequency bands: 2-50 Hz, 2-100 Hz, and 2-200 Hz.
- the magnitude of the noise is shown along vertical axis 1506 and time is shown along horizontal axis 1508.
- the noise level increases as the amount of gas in the liquid increases.
- the noise level is seen to increase more for the wider band of frequencies 1504 than for the narrower band of frequencies 1500, indicating that the noise is distributed across a wide spectrum of frequencies.
- the noise level is shown to increase 175 times for a 30% increase in gas void fraction.
- three graphs 1600, 1602 and 1604 of noise versus time show an increase in noise as the percentage of oil in a water line is increased from zero to ten percent and then to twenty percent for respective frequency bands of 2-50 Hz, 2-100 Hz, and 2-200 Hz.
- the magnitude of the noise is shown along vertical axis 1608 and time is shown along horizontal axis 1610.
- the noise increases with each increase in the percentage of oil in the water line for each frequency band.
- FIG. 18 provides a graph 1800 showing a relationship between frequency-domain determined noise and a percentage of oil added to a water flow.
- the noise magnitude is shown along vertical axis 1802 and the oil percentage is shown along horizontal axis 1804.
- Graph 1800 indicates that the noise level generally increases as the percentage of oil in the water flow increases.
- FIG. 19 provides a graph 1900 showing the relationship between frequency-domain determined noise and pounds of sand in a water flow.
- the noise magnitude is shown along vertical axis 1902 and the amount of sand is shown along horizontal axis 1904.
- Graph 1900 indicates that the noise level increases as the amount of sand increases.
- FIG. 20 provides a flow diagram of a method used by data collection module 240 to collect data for performing frequency-domain noise level identification.
- FIG. 21 provides a block diagram of elements used in the method of FIG. 20.
- analog-to-digital convertor 216 issues an interrupt indicating that a new digital sample has been produced from the magnetic flow meter sensor signal.
- a decimator 2100 applies a decimation algorithm to the sample to determine if the sample should be stored in a rolling buffer 2102. The decimating algorithm selects a subset of the samples for storage in rolling buffer 2102 thereby acting as a low pass digital filter.
- a monitor 2104 determines if enough samples have been added to rolling buffer 2102 to support a Fast Fourier Transform. If more samples are needed, the process of FIG. 20 returns to step 2000 to wait for another interrupt from analog-to-digital convertor 216.
- step 2006 the process returns to step 2000 to wait for the next interrupt from analog-to-digital convertor 216.
- FIG. 22 provides a flow diagram of a method performed by noise identification module 242 to identify the noise in the sensor signal using a frequency-domain technique.
- FIG. 23 provides a block diagram of elements used in the method of FIG. 22.
- step 2200 the start and end locations of the next set of data in rolling buffer 2102 to be processed are used to copy the data from rolling buffer 2102 to a selection buffer 2300. By copying these values, step 2200 is selecting a section or part of the sensor signal for conversion into the frequency domain.
- step 2202 the data in selection buffer 2300 is applied to a DC filter 2302, which removes the DC component from each value of the data. In accordance with one embodiment, the DC component is simply an average of all of the data in selection buffer 2300.
- the data are applied to a Hanning window 2304, which reduces the magnitudes of the data at the beginning and the end of the current section of the sensor signal to reduce frequency leakage when the Fast Fourier Transform is applied.
- the resulting data values are applied to a Fast Fourier Transform 2306, which converts the time-domain data values into a set of frequency-domain data values, with each frequency-domain data value being a complex number representing the magnitude and phase of the sensor signal for a respective frequency.
- each complex number is applied to a magnitude calculator 2308 to determine the magnitude for each frequency.
- the magnitudes are applied to a harmonic filter 2310, which removes the magnitudes for frequencies that are even or odd harmonics of the coil drive frequency.
- harmonic frequencies contain the liquid’s response to the drive signal as well as the noise in the signal due to a contaminant in the liquid.
- the noise due to a contaminant can be isolated from the remainder of the sensor signal.
- the filtered magnitudes are averaged by an average calculator 2312 and the average is stored in a noise buffer 2314 for the section of the sensor signal selected in step 2200.
- noise values in noise buffer 2314 are then applied to a contaminant identification module 244 in the same manner as discussed above for the time-domain noise values.
- the method of FIG. 11 and the block diagram of FIG. 12 can be used for the frequency-domain based noise values in the same way that they were used for the time-domain based noise values.
- the noise in the magnetic flow meter sensor signal can additionally be used to detect valve chatter.
- a relief valve in separator 100 rapidly opens and closes causing rapid fluctuations in the pressure within separator 100. This pressure fluctuation produces a corresponding fluctuation in the speed of the flow through conduits 140 and 146. Such fluctuations in the speed of the flow appear as noise in the magnetic flow meter sensor signal.
- isolating and measuring the noise in the sensor signal using either of the embodiments discussed above allows the valve chatter to be detected since the noise level of the sensor signal will increase dramatically during valve chatter.
Landscapes
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- General Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Pathology (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Immunology (AREA)
- Fluid Mechanics (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Food Science & Technology (AREA)
- Medicinal Chemistry (AREA)
- Electromagnetism (AREA)
- Oil, Petroleum & Natural Gas (AREA)
- General Chemical & Material Sciences (AREA)
- Electrochemistry (AREA)
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
- Measuring Volume Flow (AREA)
- Geophysics And Detection Of Objects (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US16/123,495 US10935402B2 (en) | 2018-09-06 | 2018-09-06 | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals |
PCT/US2019/037680 WO2020050892A1 (en) | 2018-09-06 | 2019-06-18 | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals |
Publications (2)
Publication Number | Publication Date |
---|---|
EP3830527A1 true EP3830527A1 (en) | 2021-06-09 |
EP3830527B1 EP3830527B1 (en) | 2023-07-26 |
Family
ID=67138154
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19735093.7A Active EP3830527B1 (en) | 2018-09-06 | 2019-06-18 | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals |
Country Status (5)
Country | Link |
---|---|
US (1) | US10935402B2 (en) |
EP (1) | EP3830527B1 (en) |
JP (1) | JP7126608B2 (en) |
CN (2) | CN209821150U (en) |
WO (1) | WO2020050892A1 (en) |
Families Citing this family (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US10935402B2 (en) * | 2018-09-06 | 2021-03-02 | Micro Motion, Inc. | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals |
WO2021061111A1 (en) * | 2019-09-25 | 2021-04-01 | Micro Motion, Inc. | Notification of events and apportioning of process data in a meter |
CN111780817B (en) * | 2020-06-07 | 2022-02-11 | 承德石油高等专科学校 | Algorithm for detecting and processing noise signal of low-frequency excitation electromagnetic flowmeter |
CA3191438A1 (en) * | 2020-08-13 | 2022-02-17 | Alarm.Com Incorporated | Periodic water leak detection |
DE102021208598A1 (en) * | 2021-08-06 | 2023-02-09 | Siemens Aktiengesellschaft | Noisy flow measurement method, electromagnetic flowmeter and computer program product |
CN113866259B (en) * | 2021-12-02 | 2022-03-22 | 中国核电工程有限公司 | Electromagnetic detection method and system for stainless steel pipeline weld defects |
WO2024040341A1 (en) * | 2022-08-22 | 2024-02-29 | Gea Farm Technologies Canada Inc./Division Gea Houle | Loading pipe, agricultural equipment provided with the same, kit for assembling, and corresponding methods of manufacturing, assembling and operating associated thereto |
DE102023102673B3 (en) | 2023-02-03 | 2024-05-16 | Krohne Messtechnik Gmbh | Method for operating a magnetic-inductive flow meter and a corresponding magnetic-inductive flow meter |
DE102023105640B3 (en) | 2023-03-07 | 2024-07-18 | Krohne Messtechnik Gmbh | Method for operating a magnetic-inductive flow meter and magnetic-inductive flow meter |
Family Cites Families (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3847020A (en) * | 1973-01-26 | 1974-11-12 | J Jurschak | Flow meter |
JP2856521B2 (en) | 1990-08-23 | 1999-02-10 | 株式会社日立製作所 | Electromagnetic flow meter |
JPH06300595A (en) * | 1993-04-13 | 1994-10-28 | Aichi Tokei Denki Co Ltd | Electromagnetic flowmeter |
JP3020772B2 (en) | 1993-07-09 | 2000-03-15 | 株式会社東芝 | Electromagnetic flow meter |
US6505517B1 (en) * | 1999-07-23 | 2003-01-14 | Rosemount Inc. | High accuracy signal processing for magnetic flowmeter |
JP3915459B2 (en) | 2001-09-20 | 2007-05-16 | 横河電機株式会社 | Electromagnetic flow meter |
DE102007015368A1 (en) * | 2007-03-28 | 2008-10-02 | Endress + Hauser Flowtec Ag | Method for operating a magnetic-inductive flowmeter |
DE102007052047B4 (en) * | 2007-10-31 | 2014-06-26 | Abb Ag | Method and device for measuring foreign bodies in the measuring medium |
GB2513678B (en) | 2013-04-30 | 2017-02-22 | Iphase Ltd | Oil well system and operating method including monitoring multi-phase flow in a pipe |
GB201416287D0 (en) | 2014-09-15 | 2014-10-29 | Univ Leeds | Tomography apparatus, multi-phase flow monitoring system and corresponding methods |
JP6229852B2 (en) * | 2015-03-05 | 2017-11-15 | 横河電機株式会社 | Electromagnetic flow meter |
CN108828057A (en) | 2018-06-26 | 2018-11-16 | 西安石油大学 | A kind of oil-water two-phase flow Multi-parameter detection device and method based on electromagnetism acoustical coupling |
US10935402B2 (en) * | 2018-09-06 | 2021-03-02 | Micro Motion, Inc. | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals |
-
2018
- 2018-09-06 US US16/123,495 patent/US10935402B2/en active Active
- 2018-12-04 CN CN201822027709.7U patent/CN209821150U/en active Active
- 2018-12-04 CN CN201811477029.3A patent/CN110879274B/en active Active
-
2019
- 2019-06-18 WO PCT/US2019/037680 patent/WO2020050892A1/en unknown
- 2019-06-18 EP EP19735093.7A patent/EP3830527B1/en active Active
- 2019-06-18 JP JP2021512873A patent/JP7126608B2/en active Active
Also Published As
Publication number | Publication date |
---|---|
JP2022500629A (en) | 2022-01-04 |
WO2020050892A1 (en) | 2020-03-12 |
CN110879274B (en) | 2023-01-10 |
JP7126608B2 (en) | 2022-08-26 |
CN110879274A (en) | 2020-03-13 |
US10935402B2 (en) | 2021-03-02 |
CN209821150U (en) | 2019-12-20 |
EP3830527B1 (en) | 2023-07-26 |
US20200080877A1 (en) | 2020-03-12 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US10935402B2 (en) | Fluid contaminant detection using noise levels in magnetic flow meter sensor signals | |
CN104170244B (en) | Submersible electric pump monitors and failure predication | |
CN102341720B (en) | System and method for motor fault detection using stator current noise cancellation | |
EP1877877B1 (en) | Diagnostic device for a process control system | |
US20190033898A1 (en) | System and method for assessing sand flow rate | |
GB2434645A (en) | Acoustic sand detection | |
Droubi et al. | Flow noise identification using acoustic emission (AE) energy decomposition for sand monitoring in flow pipeline | |
CN109577957A (en) | A kind of annular space flow electromagnetic measurement device and measurement method based on related transducer array | |
EP3140505B1 (en) | Anomaly fluid detection | |
GB2486799A (en) | Hydrocyclone wear monitoring | |
JP6248933B2 (en) | Leakage inspection apparatus, leakage inspection method, and leakage inspection program | |
Liu et al. | Flow regime identification for air valves failure evaluation in water pipelines using pressure data | |
WO2019040639A1 (en) | System and method for assessing sand flow rate | |
EP4165390A1 (en) | Systems and methods for continuous measurement of erosion and corrosion in oil and gas facilities | |
Durdevic et al. | Operational performance of offshore de-oiling hydrocyclone systems | |
JP2017083292A (en) | Method for determining abnormality of pipe line | |
Hansen et al. | Comparison of Inlet Observers for a De-Oiling Gravity Separator | |
Li et al. | Experimental study on inductive method for online material loss detection with high debris concentration | |
Qazi | Modelling of an axial flow compact separator using neural network |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: UNKNOWN |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE INTERNATIONAL PUBLICATION HAS BEEN MADE |
|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: REQUEST FOR EXAMINATION WAS MADE |
|
17P | Request for examination filed |
Effective date: 20210302 |
|
AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR |
|
DAV | Request for validation of the european patent (deleted) | ||
DAX | Request for extension of the european patent (deleted) | ||
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: EXAMINATION IS IN PROGRESS |
|
17Q | First examination report despatched |
Effective date: 20220509 |
|
GRAP | Despatch of communication of intention to grant a patent |
Free format text: ORIGINAL CODE: EPIDOSNIGR1 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: GRANT OF PATENT IS INTENDED |
|
INTG | Intention to grant announced |
Effective date: 20230210 |
|
GRAS | Grant fee paid |
Free format text: ORIGINAL CODE: EPIDOSNIGR3 |
|
GRAA | (expected) grant |
Free format text: ORIGINAL CODE: 0009210 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE PATENT HAS BEEN GRANTED |
|
AK | Designated contracting states |
Kind code of ref document: B1 Designated state(s): AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR |
|
REG | Reference to a national code |
Ref country code: CH Ref legal event code: EP |
|
REG | Reference to a national code |
Ref country code: DE Ref legal event code: R096 Ref document number: 602019033545 Country of ref document: DE |
|
REG | Reference to a national code |
Ref country code: IE Ref legal event code: FG4D |
|
REG | Reference to a national code |
Ref country code: LT Ref legal event code: MG9D |
|
REG | Reference to a national code |
Ref country code: NL Ref legal event code: MP Effective date: 20230726 |
|
REG | Reference to a national code |
Ref country code: AT Ref legal event code: MK05 Ref document number: 1592408 Country of ref document: AT Kind code of ref document: T Effective date: 20230726 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: NL Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: GR Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231027 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: IS Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231126 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: SE Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: RS Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: PT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231127 Ref country code: NO Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231026 Ref country code: LV Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: LT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: IS Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231126 Ref country code: HR Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: GR Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20231027 Ref country code: FI Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: AT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: PL Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: ES Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
REG | Reference to a national code |
Ref country code: DE Ref legal event code: R097 Ref document number: 602019033545 Country of ref document: DE |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: SM Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: RO Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: ES Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: EE Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: DK Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: CZ Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 Ref country code: SK Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: IT Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT Effective date: 20230726 |
|
PLBE | No opposition filed within time limit |
Free format text: ORIGINAL CODE: 0009261 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: NO OPPOSITION FILED WITHIN TIME LIMIT |
|
26N | No opposition filed |
Effective date: 20240429 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: DE Payment date: 20240521 Year of fee payment: 6 |